Clock generation for a photonic quantum computer comprising a photon-pair source to convert the converted electrical pulses into a plurality of clock signals at a first repetition rate

ABSTRACT

A system for generating clock signals for a photonic quantum computing system includes a pump photon source configured to generate a plurality of pump photon pulses at a first repetition rate, a waveguide optically coupled to the pump photon source, and a photon-pair source optically coupled to the first waveguide. The system also includes a photodetector optically coupled to the photon-pair source and configured to generate a plurality of electrical pulses in response to detection of at least a portion of the plurality of pump photon pulses at the first repetition rate and a clock generator coupled to the photodetector and configured to convert the plurality of electrical pulses into a plurality of clock signals at the first repetition rate.

CROSS REFERENCE TO RELATED APPLICATION

This application claims priority to and is a continuation ofInternational Patent Application No. PCT/US2019/038314, filed Jun. 20,2019; which claims priority to U.S. patent application Ser. No.16/362,452 filed Mar. 22, 2019, now U.S. Pat. No. 10,379,420 issued Aug.13, 2019, the entire contents of which are hereby incorporated byreference in their entirety for all purposes.

BACKGROUND OF THE INVENTION

A photonic quantum computer, such as a linear optical quantum computer(LOQC), may require the routing of photons through complex photoniccircuits that include many optical elements, such as beam splitters,phase shifters, and mirrors. Single-photon sources may be used togenerate the photons used as qubits in the quantum computing.

Despite the progress made in photonic quantum computers, there is a needin the art for improved methods and systems related to clock generation.

SUMMARY OF THE INVENTION

According to an embodiment of the present invention, a system forgenerating clock signals for a photonic quantum computing systemdisposed inside a cryostat is provided. The system includes a pumpphoton source disposed outside the cryostat. The pump photon source isconfigured to generate a plurality of pump photon pulses at a firstrepetition rate. The system also includes a waveguide optically coupledto the pump photon source and a photon-pair source disposed inside thecryostat and optically coupled to the first waveguide. The photon-pairsource is configured to receive the plurality of pump photon pulses viathe waveguide, convert a first portion of each of a subset of theplurality of pump photon pulses into a photon pair, output the photonpairs converted from the subset of the plurality of pump photon pulses,and output a second portion of each pump photon pulse of the pluralityof pump photon pulses. The system further includes a photodetectordisposed inside the cryostat and configured to receive the secondportion of each pump photon pulse of the plurality of pump photon pulsesgenerate a plurality of electrical pulses by converting the secondportion of each pump photon pulse of the plurality of pump photon pulsesinto a respective electrical pulse of the plurality of electricalpulses. Moreover, the system includes a clock generator disposed insidethe cryostat and electrically coupled to the photodetector. The clockgenerator is configured to convert the plurality of electrical pulsesgenerated by the photodetector into a plurality of clock signals at thefirst repetition rate.

According to another embodiment of the present invention, a system forgenerating clock signals for a photonic quantum computing system isprovided. The system includes a pump photon source configured togenerate a plurality of pump photon pulses at a first repetition rate, awaveguide optically coupled to the pump photon source, and a photon-pairsource optically coupled to the first waveguide. The system alsoincludes a photodetector optically coupled to the photon-pair source andconfigured to generate a plurality of electrical pulses in response todetection of at least a portion of the plurality of pump photon pulsesat the first repetition rate and a clock generator coupled to thephotodetector and configured to convert the plurality of electricalpulses into a plurality of clock signals at the first repetition rate.In an embodiment, a second portion of each pump photon pulse of theplurality of pump photon pulses is output by the first waveguide and thephotodetector is optically coupled to the first waveguide.

According to an alternative embodiment of the present invention, amethod of generating clock signals for a photonic quantum computingsystem disposed inside a cryostat is provided. The method includesgenerating, using a pump photon source disposed outside the cryostat, aplurality of pump photon pulses at a first repetition rate, andconverting, using a photon-pair source disposed inside the cryostat andoptically coupled to the pump photon source via a waveguide, a firstportion of each of a subset of the plurality of pump photon pulses intoa photon pair. The photon-pair source outputs a second portion of eachpump photon pulse of the plurality of pump photon pulses. The methodalso includes generating, using a photodetector disposed inside thecryostat, a plurality of electrical pulses by converting the secondportion of each pump photon pulse of the plurality of pump photon pulsesinto a respective electrical pulse of the plurality of electrical pulsesand generating, using a clock generator disposed inside the cryostat andcoupled to the photodetector, a plurality of clock signals at the firstrepetition rate using the plurality of electrical pulses.

In an embodiment, the photon-pair source, the photodetector, the clockgenerator, and the photonic quantum computing system are disposed on asingle chip placed inside the cryostat. The photon pair can include asignal photon and a heralding photon. One of the signal photon or theheralding photon is used by the quantum computing system as a qubit. Inan exemplary embodiment, the first portion of each of the subset of theplurality of pump photon pulses is converted into the photon pairnon-deterministically.

In an embodiment, the photon-pair source comprises a first waveguideoptically coupled to the pump photon source via the waveguide forreceiving the plurality of pump photon pulses; a resonator opticallycoupled to the first waveguide and comprising a nonlinear opticalmaterial; and a second waveguide optically coupled to the resonator. Theresonator can include one or more ring resonators. In this embodiment,the method further comprises coupling a portion of each pump photonpulse of the plurality of pump photon pulses from the first waveguideinto the resonator. The first portion of each of the subset of theplurality of pump photon pulses that is converted into the photon pairis among the portion and is converted by the nonlinear optical materialof the resonator. The method also includes coupling the photon pairsconverted from the subset of the plurality of pump photon pulses by theresonator into the second waveguide.

In another embodiment, the second portion of each pump photon pulse ofthe plurality of pump photon pulses is among the portion and the methodfurther comprises coupling the second portion of each pump photon pulseof the plurality of pump photon pulses from the resonator into thesecond waveguide. In some embodiment, the method also includesseparating, using a pump rejecter disposed inside the cryostat andoptically coupled to the second waveguide, the second portion of eachpump photon pulse of the plurality of pump photon pulses from the photonpairs and coupling the second portion of each pump photon pulse of theplurality of pump photon pulses into the photodetector to be convertedinto the plurality of electrical pulses. As an example, the pumprejecter can include a spectral filter.

In yet another embodiment, the second portion of each pump photon pulseof the plurality of pump photon pulses is among a remaining portion ofeach pump photon pulse of the plurality of pump photon pulses that isnot coupled into the resonator, In this embodiment, the method furtherincludes coupling the second portion of each pump photon pulse of theplurality of pump photon pulses from the first waveguide into thephotodetector to be converted into the plurality of electrical pulses.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1A shows a hybrid computing system in accordance with one or moreembodiments.

FIG. 1B shows a block diagram of a hybrid QC system 101 in accordancewith some embodiments.

FIG. 2 is a simplified block diagram of an example of a single-photonsource that may include a set of cascaded heralded photon sources(HPS's) according to some embodiments.

FIG. 3 illustrates an example of a photon-pair source according to someembodiments.

FIG. 4 illustrates an example of a single-photon source that includesseveral HPS's that are multiplexed according to some embodiments.

FIG. 5A illustrates schematically a train of pump photon pulses thatarrive at the HPS's shown in FIG. 4 according to some embodiments.

FIG. 5B illustrates the non-deterministic manner in which the HPS'sillustrated in FIG. 4 generate single photons.

FIG. 6 illustrates a schematic block diagram of a system for generatingclock signals for a photonic quantum computer according to someembodiments.

FIG. 7 a schematic block diagram of a system for generating clocksignals for a photonic quantum computer according to some otherembodiments.

FIG. 8 a schematic block diagram of an alternative system for generatingclock signals for use by a single photon detector according to someembodiments.

FIG. 9 a schematic block diagram of an alternative system for generatingclock signals for use by a single photon detector according to someother embodiments.

FIG. 10 shows a simplified flowchart illustrating a method forgenerating clock signals for a photonic quantum computing systemaccording to some embodiments.

FIG. 11 is a cross-sectional view of a package that includes a photonicintegrated circuit and an electronic integrated circuit according tocertain embodiments.

FIG. 12A is a simplified schematic diagram illustrating a systemincluding a clock signal generator according to an embodiment of thepresent invention.

FIG. 12B is a set of plots illustrating optical and electrical signalsassociated with various elements of the system illustrated in FIG. 12A.

FIG. 13 is a simplified schematic diagram illustrating generation of aclock signal in conjunction with two or more photon-pair sources.

DETAILED DESCRIPTION OF SPECIFIC EMBODIMENTS

In some photonic quantum computers, the various optical elements may beremote from one another, and yet need to be operated with very precisetiming. To achieve precise timing control, an accurate system clock maybe required. Thus, embodiments of the present invention provide systemsand methods of generating clock signals for a photonic quantum computingsystem.

A photonic quantum computer, e.g., such as the systems shown in FIGS.1A-1B below, may require an accurate system clock to control the timingof the operations of various optical elements. The system clock may needto have characteristics such as low phase noise, small drift, and thelike, for achieving high performance of the photonic quantum computer.The system clock may be set according to the photon generation rate ofthe single-photon sources. While one may desire to recover the systemclock from the photon stream in a manner analogous to classical clockrecovery from a data stream, this option is not available for a photonicquantum computer, because doing so would require the measurement andthus destruction of the same photons that are used to perform thequantum computing (i.e., the photonic qubits). Thus, generating anaccurate clock for a photonic quantum computer may pose particularchallenges.

FIG. 1A shows a hybrid computing system in accordance with one or moreembodiments. The hybrid computing system 101 includes a user interfacedevice 104 that is communicatively coupled to a hybrid quantum computing(QC) sub-system 106, described in more detail below in FIG. 1B. The userinterface device 104 can be any type of user interface device, e.g., aterminal including a display, keyboard, mouse, touchscreen and the like.In addition, the user interface device can itself be a computer such asa personal computer (PC), laptop, tablet computer and the like. In someembodiments, the user interface device 104 provides an interface withwhich a user can interact with the hybrid QC subsystem 106. For example,the user interface device 104 may run software, such as a text editor,an interactive development environment (IDE), command prompt, graphicaluser interface, and the like so that the user can program, or otherwiseinteract with, the QC subsystem to run one or more quantum algorithms.In other embodiments, the hybrid QC subsystem 106 may be pre-programmedand the user interface device 104 may simply be an interface where auser can initiate a quantum computation, monitor the progress, andreceive results from the hybrid QC subsystem 106. Hybrid QC subsystem106 further includes a classical computing system 108 coupled to one ormore quantum computing chips 110. In some examples, the classicalcomputing system 108 and the quantum computing chips 110 can be coupledto other electronic and/or optical components 112, e.g., pulsed pumplasers, microwave oscillators, power supplies, networking hardware, etc.In some embodiments that require cryogenic operation, the quantumcomputing chips 110 can be housed within a cryostat, e.g., cryostat 114.On other embodiments where cryogenic operation is not required, thequantum computing chips 110, the cryostat 114 may be replaced with anyother enclosure. In some embodiments, the quantum computing chips 110can include one or more constituent chips, e.g., hybrid controlelectronics 116 and integrated photonics chip 118. Signals can be routedon- and off-chip any number of ways, e.g., via optical interconnects 120and via other electronic interconnects 122. In addition, the hybridcomputing system 101 may employ a quantum computing process, e.g.,measurement-based quantum computing (MBQC), circuit-based quantumcomputing (CBQC) or any other quantum computing scheme.

FIG. 1B shows a block diagram of a hybrid QC system 101 in accordancewith some embodiments. Such a system can be associated with the hybridcomputing system 101 introduced above in reference to FIG. 1A 1. In FIG.1B, solid lines represent quantum information channels and dashedrepresent classical information channels. The hybrid QC system 101includes a qubit entangling system 103, qubit readout system 105, andclassical computing system 107. In some embodiments, the qubitentangling system 103 takes as input a collection of N physical qubits,e.g., physical qubits 109 (also represented schematically as inputs 111a, 111 b, 111 c, . . . , 111 n) and generates quantum entanglementbetween two or more of them to generate an entangled state 115. Forexample, in the case of photonic qubits, the qubit entangling system 103can be a linear optical system such as an integrated photonic circuitthat includes waveguides, beam splitters, photon detectors, delay lines,and the like. In some examples, the entangled state 115 can be alattice, cluster, or graph state, or one part of a larger lattice,cluster, or graph state that is created over the course of several clockcycles of the quantum computer. In some embodiments, the input qubits109 can be a collection of quantum systems and/or particles and can beformed using any qubit architecture. For example, the quantum systemscan be particles such as atoms, ions, nuclei, and/or photons. In otherexamples, the quantum systems can be other engineered quantum systemssuch as flux qubits, phase qubits, or charge qubits (e.g., formed from asuperconducting Josephson junction), topological qubits (e.g., Majoranafermions), or spin qubits formed from vacancy centers (e.g., nitrogenvacancies in diamond). Furthermore, for the sake of clarity ofdescription, the term “qubit” is used herein although the system canalso employ quantum information carriers that encode information in amanner that is not necessarily associated with a binary bit. Forexample, qudits can be used, i.e., quantum systems that can encodeinformation in more than two quantum states in accordance with someembodiments.

In accordance with some embodiments, the hybrid QC system 101 can be aquantum circuit-based quantum computer, a measurement-based quantumcomputer, or any other type of quantum computer. In some embodiments, asoftware program (e.g., a set of machine-readable instructions) thatrepresents the quantum algorithm to be run on the hybrid QC system 101can be passed to a classical computing system 107 (e.g., correspondingto system 108 in FIG. 1A above). The classical computing system 107 canbe any type of computing device such as a PC, one or more blade servers,and the like, or even a high-performance computing system such as asupercomputer, server farm, and the like. Such a system can include oneor more processors (not shown) coupled to one or more computer memories,e.g., memory 106. Such a computing system will be referred to herein asa “classical computer.” In some examples, the software program can bereceived by a classical computing module, referred to herein as adetection pattern generator 113. One function of the detection patterngenerator 113 is to generate a set of machine-level instructions fromthe input software program (which may originate as code that can be moreeasily written by a user to program the quantum computer), i.e., thedetection pattern generator 113 can operate as a compiler, logicprocessor, and/or encoder to allow software programs to be run on thequantum computer. Detection pattern generator 113 can be implemented aspure hardware, pure software, or any combination of one or more hardwareor software components or modules. In some examples, the compiledmachine-level instructions take the form of one or more data frames thatinstruct the qubit readout circuit to make one or more quantummeasurements on the entangled state 115. Measurement pattern 117 (e.g.,a data frame) is one example of the set of measurements and/or gatesthat should be applied to the qubits of entangled state 115 during acertain clock cycle as the program is executed. In other examples, e.g.,the measurement pattern 117 can include instructions for applyingmulti-qubit measurements and/or multi-qubit gates, e.g., in the casewhere a fusion gate is desired to be applied to two or more qubits orwhen stabilizer measurements are being performed. In some embodiments,several measurement patterns 117 can be stored in memory 106 asclassical data. Generally, the measurement patterns 117 can dictatewhether or not a detector from the qubit detection array 121 of thequbit readout circuit 105 should make a measurement on a given qubitthat makes up the entangled state 115. In addition, the measurementpattern 117 can also store which basis (e.g., Pauli X, Y, Z, etc.) themeasurement should be made in order to execute the program. In someexamples, the measurement pattern 117 can also include a set of gatesthat should be applied by the qubit entangling circuit to the next setof physical qubits 109 that are to be processed at some future clockcycle of the hybrid QC system 101.

A controller circuit 119 of the qubit readout circuit 105 can receivedata that encodes the measurement pattern 117 and generate theconfiguration signals necessary to drive a set of detectors within thequbit detection array 121. The detectors can be any detector that candetect the quantum states of one or more of the qubits in the entangledstate 115. For example, for the case of photonic qubits, the detectorscan be single photon detectors that are coupled to one or morewaveguides, beam splitters, interferometers, switches, polarizers,polarization rotators and the like. One of ordinary skill willappreciate that many types of detectors may be used depending on theparticular qubit architecture.

In some embodiments, the result of applying the detection pattern 117 tothe qubit detection array is a readout operation that “reads out” thequantum states of the qubits in the entangled state 115. Once thismeasurement is accomplished, the quantum information stored within theentangled state 115 is converted to classical information thatcorresponds to a set of eigenvalues that are measured by the detectors,referred to herein as “measurement outcomes.” These measurement outcomescan be stored in a measurement outcome data frame, e.g., data frame 122and passed back to the classical computing system for furtherprocessing.

In some embodiments, any of the submodules in the hybrid QC system 101,e.g., controller 123, quantum gate array 125, detection array 121,controller 119, detection pattern generator 113, decoder 133, andlogical processor 108 can include any number of classical computingcomponents such as processors (CPUs, GPUs, TPUs) memory (any form ofRAM, ROM), hard coded logic components (classical logic gates such asAND, OR, XOR, etc.) and/or programmable logic components such as fieldprogrammable gate arrays (FPGAs and the like). These modules can alsoinclude any number of application specific integrated circuits (ASICs),microcontrollers (MCUs), systems on a chip (SOCs), and other similarmicroelectronics.

As described herein, the logical qubit measurement outcomes 127 can befault tolerantly recovered, e.g., via decoder 133, from the measurementoutcomes 122 of the physical qubits. In the case of a cluster state thatis also a stabilizer state, the error syndrome generated by themeasurement of joint parity measurements (formed from the combination ofone or more stabilizer measurements) are used by the decoder to identifyand correct errors so that the correct logical qubit measurement outcomecan be determined. Logical processor 108 can then process the logicaloutcomes as part of the running of the program. As shown, the logicalprocessor 108 can feed back information to the detection patterngenerator 113 to affect downstream gates and/or measurements to ensurethat the computation proceeds fault tolerantly.

In accordance with some embodiments, it may be beneficial tosynchronize, or otherwise coordinate in time, the actions of any or allof the components of the hybrid QC system. Advantageously, one or moreembodiments provide systems and methods for clock signal generation anddistribution using residual light (i.e., photons) from a train of pulsesoriginating from the pump laser, e.g., housed within electronic and/oroptical components 112 shown in FIG. 1A.

In the description that follows, embodiments are described that employspatial modes of photons as the qubit system, but one of ordinary skillwill appreciate that any type of qubit described by any type of mode canbe employed without departing from the scope of the present disclosure.Furthermore, in what follows, photonic waveguides are used to define thespatial modes of the photon. However, one of ordinary skill having thebenefit of this disclosure will appreciate that any type of mode, e.g.,polarization modes, temporal modes, and the like, can be used withoutdeparting from the scope of the present disclosure. The diagrams shownin the remaining figures are schematic diagrams with each horizontalline representing a mode of a quantum system, e.g., a waveguide.

FIG. 2 is a simplified block diagram of an example of a single-photonsource 200 that may include a set of cascaded HPS's according to someembodiments. In the example shown in FIG. 2 , the single-photon source200 may include multiple HPS's 205 a, 205 b, and the like, which may becollectively referred to as HPS's 205. Each HPS 205 may include aphoton-pair source, such as the photon-pair source 210 a in HPS 205 a orthe photon-pair source 210 b in HPS 205 b. Each photon-pair source 210 aor 210 b may generate a pair of photons based on, for example,spontaneous four wave mixing (SFWM) in third-order passive nonlinearoptical materials or spontaneous parametric down-conversion (SPDC) insecond-order passive nonlinear optical materials. In someimplementations, a photon-pair source 210 a or 210 b may include a ringresonator that may support multiple resonances as described below.

It will be appreciated that although some embodiments are described inrelation to a photon-pair source, this is not required and photonsources other than photon-pair sources are included within the scope ofthe present invention. Thus, for the sake of illustration, amicroring-based SPFW heralded photon source (HPS) is described as anexample of the source of photons. However, the precise type of photonsource used is not critical and any type of nonlinear source, employingany process, such as SPFW, spontaneous parametric down-conversion(SPDC), or any other process can be used. Other classes of sources thatdo not necessarily require a nonlinear material can also be employed,such as those that employ atomic and/or artificial atomic systems can beused, e.g., quantum dot sources, color centers in crystals, and thelike.

In some cases, sources may or may be coupled to photonic cavities, e.g.,as can be the case for artificial atomic systems such as quantum dotscoupled to cavities. Other types of photon sources also exist for SPWMand SPDC, such as optomechanical systems and the like.

For the sake of illustration, an example which employs spatialmultiplexing of several non-deterministic is described as an example ofa multiplexed (MUX) photon source. However, many different spatial MUXarchitectures are possible without departing from the scope of thepresent disclosure. Temporal MUXing can also be implemented instead ofor in combination with spatial multiplexing. MUX schemes that employlog-tree, generalized Mach-Zehnder interferometers, multimodeinterferometers, chained sources, chained sources with dump-the-pumpschemes, asymmetric multi-crystal single photon sources, or any othertype of MUX architecture can be used. In some embodiments, the photonsource can employ a MUX scheme with quantum feedback control and thelike.

In each photon-pair source 210 a or 210 b, photons may benon-deterministically produced in pairs, where each pair includes asignal photon and an idler photon, the existence of one photon (e.g.,the idler photon) may indicate the existence of the other photon (e.g.,the signal photon) in the pair. The two photons in each pair may beseparated to two output channels by a splitter, for example a wavelengthdivision demultiplexing (WDDM) device 220 a or 220 b, based on theirdifferent frequencies. One photon (e.g., the idler photon) on one outputchannel of the splitter (e.g., WDDM device 220 a or 220 b) may bedetected by a single photon detector (SPD) 230 a or 230 b. If a photonis detected by an SPD 230 a or 230 b, a corresponding photon (e.g., thesignal photon) that is generated in the same pair as the detected photonwould exist on a different output channel of the splitter 220 a or 220b, and thus can be used as the output of the single-photon source 200.When an idler photon is detected by an SPD 230 a or 230 b in one of thecascaded HPS's 2050 a and 205 b, the SPD 230 a or 230 b may send anelectrical signal (referred herein as a heralding signal) to the otherHPS's, so that those HPS's may be switched off or bypassed. Forinstance, in the example shown in FIG. 2 , if a photon is detected bythe SPD 230 a in the first HPS 205 a, the SPD 230 a may send a heraldingsignal to the second HPS 205 b, so that the second HPS 205 b may beturned off or bypassed. The signal photon generated by the first HPS 205a may pass through the second HPS 205 b as an output of single-photonsource 200.

FIG. 3 illustrates an example of a photon-pair source 300 according tosome embodiments. The photon-pair source 300 may include a firstwaveguide 310, a second waveguide 330, and a ring resonator 320positioned between the first waveguide 310 and the second waveguide 330.Pump light (e.g., generated by a laser source) may be propagated in thefirst waveguide 310 (as indicated by the arrow), and may be coupled intothe ring resonator 320. The ring resonator 320 may include a waveguideloop such that a resonance for light having a certain wavelength mayoccur when the optical path length of the ring resonator 320 is aninteger number of the wavelength of the light. The ring resonator 320may support multiple resonances at multiple wavelengths that may meetthe resonance condition. The spacing between these resonances may bereferred to as the free spectral range (FSR) and may depend on theoptical path length of the ring resonator 320.

The ring resonator 320 may include a nonlinear optical material, such asa second-order or third-order passive nonlinear optical medium.Spontaneous four wave mixing (SFWM) or spontaneous parametricdown-conversion (SPDC) process may occur in the ring resonator 320. Inan SFWM process, two pump photons may be converted into a pair ofdaughter photons (e.g., a signal photon and an idler photon) in thenonlinear optical material. Due to energy conservation, the signalphoton and the idler photon may be at frequencies that are symmetricallydistributed around the pump frequency (e.g., one at frequency f₀+Δf, theother one at frequency f₀−Δf, where f₀ is the frequency of pumpphotons).

The signal photon and the idler photon generated within the ringresonator 320 may be coupled out of the ring resonator 320 into thesecond waveguide 330 at a certain coupling efficiency. The propagationdirections of the photons in the first waveguide 310, the ring resonator320, and the second waveguide 330 may be as shown by the arrows in FIG.3 . In addition to photon pairs that are generated by the resonator 320,certain amount of unconverted pump photons may also be coupled from thering resonator 320 into the second waveguide 330.

The photon-pair source 300 may generate photon pairs in anon-deterministic manner. That is, the photon pairs are not generatedon-demand, but instead are generated probabilistically. The success ratemay be only 1-5%. For example, a photon pair may be successfullygenerated only once in every 20 pump pulses. As a result, a heraldedphoton source (HPS) that uses a photon-pair source 300 to generatesingle photons (e.g., the HPS 205 a or 205 b illustrated in FIG. 2 ) mayalso generate single photons in a non-deterministic manner. According tosome embodiments, multiple HPS's may be cascaded (e.g., as illustratedin FIG. 2 ), or multiplexed to form a quasi-deterministic single-photonsource, as described below.

FIG. 4 shows, as an example, a single-photon source 400 that includesthree HPS's 410 a-410 c that are multiplexed. Pump photon pulses (e.g.,laser pulses) are distributed to each HPS 410 a, 410 b, and 410 c, forexample, simultaneously. The outputs of the HPS's 410 a-410 c arecoupled to a multiplexer (MUX) 420. FIG. 4 shows a single-photon source400 that includes three HPS's for illustration purposes, a single-photonsource may include twenty or more HPS's in some embodiments.

Each of the HPS's 410 a-410 c may generate single photons in anon-deterministic manner. For example, FIG. 5A illustrates schematicallya train of pump photon pulses that arrive at the HPS's 410 a, 410 b, and410 c at time slots t₁, t₂, and t₃. As illustrated in FIG. 5B, the firstHPS 410 a may not generate any single photon at the first time slot t₁and the third time slot t₃ (indicated by the crosses), but may generatea single photon at the second time slot t₂ (indicated by the checksymbol). Similarly, the second HPS 410 b may not generate any singlephoton at the first time slot t₁ and the second time slot t₂, but maygenerate a single photon at the third time slot t₃; and the third HPS410 c may not generate any single photon at the second time slot t₂ andthe third time slot t₃, but may generate a single photon at the firsttime slot t₁.

When an idler photon is detected (e.g., by a single-photon detector) ina HPS 410 a, 410 b, or 410 c, the HPS 410 a, 410 b, or 410 c may send aheralding signal to the multiplexer 420. The multiplexer 420 may beconfigured to select the single-photon output of one of the HPS's 410 a,410 b, and 410 c as its single photon output, and ignore thesingle-photon outputs of all other HPS's. When there are sufficientnumber of HPS's, the single-photon source 400 may be able to produce asingle photon for each pump photon pulse in a quasi-deterministicmanner. For instance, in the example illustrated in FIGS. 4 and 5A-5B,the multiplexer 420 may select the single-photon output of the third HPS410 c at the first time slot t₁, the output of the first HPS 410 a atthe second time slot t₂, and the output of the second HPS 410 b at thethird time slot t₃, so that the single-photon source 400 outputs asingle phone for each of the pump photon pulses at time slots t₁, t₂,and t₃.

In order for the system to deterministically sequence the multipleoperations of the various components, including, e.g., one or moresingle-photon sources like 400 a, 400 b, 400 c, one or more MUXes likeMUX 420, and/or any other downstream components, such as any or all ofthose components shown in FIGS. 1A-1B, a shared, or master, clock signalmay be beneficial. Accordingly, in some embodiments, the clock signalgenerator 450 can convert a portion of the pump photon pulses to a clocksignal that then can be distributed to the various components to conductthe desired coordination between components. While the portion of thepump signal used to derive the clock signal shown in FIG. 4 is derivedfrom an output of a single photon source, the portion can be providedfrom any number different upstream or combination of blocks withoutdeparting from the scope of the present disclosure.

Referring again to FIG. 1B, the physical qubit inputs 111 a, 111 b, 111c, . . . , 111 n can be single photons generated by upstreamsingle-photon sources (not shown) and may be coupled into the qubitentangling system 103, which in this example may be, e.g., a complexlinear optical circuit (e.g., there may be up to a million qubits). Forexample, the linear optical quantum circuit may include opticalcomponents such as switches, beamsplitters, phase shifters, photondetectors that need to be coordinated in order to entangle two or moresingle photons or two or more entangled cluster states of photons. Thelinear optical quantum circuit may include quantum gates (e.g., fusiongates) at various locations to perform the quantum computing. The QubitReadout System 105 can include many single-photon measurement circuitsand also may include many photon fusion circuits (e.g., type I and/ortype II fusion gates) which can measure the photons to obtain results ofthe quantum computing. In some architectures, the quantum gatesthemselves can be formed/defined by a sequence of measurement and/orfusion operations that are to be performed on the individual photons. Ineither case, there are a number of operations within the quantumcomputer that may need to be precisely timed. Thus, a precise systemclock may be needed to serve as a “master conductor” to control thetiming of various operations of the quantum computer 101.

In some embodiments, the system clock may be set by the photongeneration rate of the single-photon sources. The single-photon sourcesmay be driven by a high-power pump laser that produces a train of pumpphoton pulses at certain repetition rate (e.g. square wave pulses at 100ps spacing, corresponding to a repetition rate of about 10 GHz). Thehigh-power pump laser may in turn be driven by an electrical signalhaving a similar repetition rate. Thus, one option for generating aclock signal is to tap off some of the electrical signals that generatethe pump photon pulses and pipe it to the linear optical quantumcomputer 101 to be used as a master clock. Unfortunately, this optionmay not work for one or more of the reasons discussed below.

As discussed above, many components of the linear optical quantumcomputer 101 may be implemented on a chip, which is placed inside acryostat so as to keep those components at a cryogenic temperature forachieving high performances. On the other hand, the electrical circuitrythat drives the pump photon source (e.g., a power laser source) may beremotely located from the chip and may be at room temperature. As such,there may be electrical and optical interconnects between the pumpphoton source and the linear optical quantum computer 101 that aresubject to very different temperature environments (e.g., from roomtemperature of about 293 K to about 4 K inside the cryostat). As aresult, a master clock generated in this way may have random phaseerrors. Because of the tight timing tolerances required by a linearoptical quantum computer, the phase errors may render such as masterclock unsuitable for use for the linear optical quantum computer.

Another approach to generate a clock signal is to generate clock signalsfrom the heralding signals when idler photons are detected in a heraldedphoton source (HPS). This approach, however, may not work either. Asdiscussed above, a HPS may generate single-photons in anon-deterministic manner. The success rate may be only 1-5% (e.g., onlyone single photon is generated for every 20 pump photon pulses). Thus,the heralding signal rate may be a lot slower than the pump pulse rate.The slow rate and the non-deterministic nature of the heralding signalsmake them unsuitable for recovering clock signals therefrom.

Embodiments of the present invention provide methods of generating clocksignals for a photonic quantum computer that utilize the excess pumpphotons rejected by the single-photon sources that generate thesingle-photon qubits for the photonic quantum computer. The excess pumpphotons would ordinarily be wasted and dumped out of the system. Bygenerating clock signals locally on the chip where the photonic quantumcomputer resides, which is usually placed inside a cryostat, randomphase errors may be prevented or reduced.

FIG. 6 illustrates a schematic block diagram of a system for generatingclock signals for a photonic quantum computer according to someembodiments. The system may include a pump photon source 602 and aphoton-pair source 610. The pump photon source 602 may be configured togenerate a train of pump photon pulses to be coupled into thephoton-pair source 610 via a waveguide 604, such as an optical fiber.The train of pump photon pulses may have a repetition rate of, forexample, 10 GHz and the like.

The photon-pair source 610 may reside on a chip that is placed inside acryostat (e.g., at a cryogenic temperature). The pump photon source 602may reside remotely from the chip at room temperature. The waveguide 604may be configured to have certain length so as to cause a desired timedelay for the train of light pulses.

The photon-pair source 610 may be similar to the photon-pair source 300illustrated in FIG. 3 according to some embodiments. For example, thephoton-pair source 610 may include a first waveguide 614, a secondwaveguide 616, and a resonator 612 (e.g., one or more ring resonators).The pump photons are coupled into the first waveguide 614, some of whichare coupled into the resonator 612. The resonator 612 may include anonlinear optical material that may convert two pump photons into a pairof photons, one being a signal photon (S), the other being an idlerphoton or heralding photon (H). A majority of the pump photons that arecoupled into the ring resonator 612 may be unconverted, which arereferred herein as excess pump photons. The converted pairs of signalphoton and heralding photon, as well as the excess pump photons, may becoupled into the second waveguide 616 and be output from the photon-pairsource 610. In addition, a portion of the pump photons that are coupledinto the first waveguide 614 may not be coupled into the ring resonator612. These pump photons are referred herein as non-coupled pump photons.The non-coupled pump photons may be absorbed by a beam dump (not shown).

As discussed below in relation to FIG. 7 , in addition to the clockgeneration architecture illustrated in FIG. 6 , alternative embodimentsutilize all or a portion of the non-coupled pump photons during theclock generation process. Moreover, combinations in which coupled pumpphotons in addition to or in place of non-coupled pump photons areutilized are included within the scope of the present invention. One ofordinary skill in the art would recognize many variations,modifications, and alternatives.

The system may further include a pump rejecter 620 coupled to the outputof the photon-pair source 610. The pump rejecter 620 may be configuredto separate the excess pump photons from the converted pairs of signalphoton and idler photon. Since the signal photon and idler photon mayhave different frequencies from that of the excess pump photons, thepump rejecter 620 may include a spectral filter configured to separatethe excess pump photons from the signal photons and the idler photonsspectrally. For example, assuming that the frequency of the pump photonsis f₀, the signal photon and the idler photon may have frequencies f₀+Δfand f₀−Δf, respectively. The pump rejecter 620 may include a notchfilter that passes the signal photon and the idler photon at theirrespective frequencies and send the pump photons at frequency f₀ along adifferent path. As discussed above, a majority of the pump photons in apump photon pulse (e.g., in the order of 10¹⁰ photons per 10 pJ pulse)may be unconverted.

Similar to the heralded photon source (HPS) 205 a illustrated in FIG. 2, the signal photon (S) and the idler photon (H) may be passed onto awavelength division demultiplexing (WDDM) device 630, which separatesthe signal photon and the idler photon spectrally. The idler photon (H)may be detected by a single-photon detector (SPD) 640. The single-photondetector 640 may send a heralding signal (electrical signal) to amultiplexer 650 when it detects an idler photon, so that the multiplexer650 may couple the signal photon (S) to its output to be used a qubitfor the photonic quantum computer, and bypass or ignore the outputs ofother HPS's coupled to the multiplexer 650 (not shown in FIG. 6 ).

The system may further include a photodetector 670 and a clock generator660. The photodetector 670 is optically coupled to the pump rejecter 620for receiving the excess pump photons rejected by the pump rejecter 620.The photodetector 670 may convert the excess pump photons intoelectrical pulses. The electrical pulses are in turn input into theclock generator 660, which generates clock signals from the electricalpulses. In some embodiments, the clock generator 660 may include anoptoelectronic amplifier that amplifies the electrical pulses generatedby the photodetector 670 to generate the clock signals 662 and 664.

In some embodiments, photodetector 670 may be integrated with clockgenerator 660. Thus, embodiments in which photodetector 670 isintegrated with clock generator 660 as well as embodiments in whichphotodetector 670 is implemented separately, e.g., as a separateelement, from clock generator 660 are included within the scope of theinvention. One of ordinary skill in the art would recognize manyvariations, modifications, and alternatives.

FIG. 12A is a simplified schematic diagram illustrating a systemincluding a clock signal generator according to an embodiment of thepresent invention. FIG. 12B is a set of plots illustrating optical andelectrical signals associated with various elements of the systemillustrated in FIG. 12A. The clock signal generator 1230 illustrated inFIG. 12A can be utilized as any of the clock signal generators describedin this application, for example, clock generator 660, clock generator760, clock generator 860, or clock generator 960. As illustrated in FIG.12A, the system includes a pump photon source 1210 and a photon-pairsource 1212, which can be compared to pump photon source 602 andphoton-pair source 610 in FIG. 6 , respectively. Referring to FIG. 12B,the optical signal, e.g., optical pulses, delivered by pump photonsource 1210 is illustrated as the plot for the pump in FIG. 12B.

Excess pump photons are delivered to detector 1220, which can becompared to photodetector 670 in FIG. 6 . Detector 1220 converts theexcess pump photons into electrical pulses. Referring to FIG. 12B, theelectrical pulses output by detector 1220 are illustrated as plot “a”,i.e., Detector Current. Clock signal generator 1230 receives theelectrical pulse output by detector 1220 and includes a transimpedanceamplifier (TIA) 1232 and a limiting amplifier 1234. The output of theTIA 1232 is illustrated as plot “b” in FIG. 12B, i.e., TIA Output. Thelimiting amplifier 1234 thus outputs the clock signal “ck” illustratedin FIG. 12B, i.e., Limiting Amp Output. The clock signal “ck” can beconsidered as the recovered electrical clock from the pump photon sourceand provided to electrical circuits 1240 as described herein.

FIG. 11 is a cross-sectional view of a package that includes a photonicintegrated circuit and an electronic integrated circuit according tocertain embodiments. Referring to FIG. 11 , package 1100 includes aphotonic integrated circuit (PIC) die 1130, also referred to as a PICwafer, an electronic integrated circuit (EIC) die 1140, a PCB 1120, oneor more electrical connectors 1122, and optical fibers 1150 on a siliconhandle wafer 1110. Even though FIG. 11 only shows one PIC/EIC die stack,multiple PIC/EIC die stacks may be included in package 1100. Asillustrated, a PCB 1120 is attached to silicon handle wafer 1110, e.g.,using an epoxy or through fusion bonding or hybrid bonding, depending onthe material of PCB 1120. One or more PCBs 1120 may be attached tosilicon handle wafer 1110 at different horizontal or vertical locations.A PIC/EIC die stack includes EIC die 1140 bonded face-to-face with PICdie 1130 (e.g., by fusion bonding or hybrid bonding) such that the PICsmay directly face the EICs. The PIC/EIC die stack may be bonded tosilicon handle wafer 1110 by, for example, fusion bonding. EIC die 1140may be electrically connected to PCB 1120 through bonding wires 1142,where the bonding pads and bonding wires may only be at the top andbottom sides of the PIC/EIC die stack. The left and right sides of thePIC/EIC die stack may be coupled with optical fibers, which may beattached to PCB 1120 through harnesses. PCB 1120 may also includeelectrical connectors 1122 and some other electronic components, such asvoltage regulators, power management ICs, decoupling capacitors, etc.

In the cross-sectional view illustrated in FIG. 11 , PCB 1120 and thePIC/EIC die stack are bonded to a top surface of silicon handle wafer1110. PCB 1120 may include multiple layers of interconnect traces orplanes connected through vias. Electronic components, such as electricalconnector 1122 and decoupling capacitors 1124 may be soldered on the topsurface of PCB 1120. PCB 1120 may also include solder pads 1126 on thetop surface of PCB 1120.

The PIC/EIC die stack may include PIC die 1130 and EIC die 1140. PIC die1130 may include a back surface 1133 bonded to silicon handle wafer1110. PIC die 1130 may also include a front surface 1131 that mayinclude circuits or pads. EIC die 1140 may include a back surface 1143that may include a redistribution layers (RDL) and bonding pads 1148.EIC die 1140 may also include a front surface 1141 that may includecircuits or pads. EIC die 1140 and PIC die 1130 may be bondedface-to-face with each other such that front surface 1131 of PIC die1130 and front surface 1141 of EIC die 1140 may directly face each otherand the interconnections can be short. PIC die 1130 may includewaveguides 1132 and 1136, and photodetectors 1134. EIC die 1140 mayinclude some through-silicon vias (TSVs) 1146 and control logic circuits1144. A photodetector 1134 may detect a single photon from waveguide1132, and send the detection result to control logic circuit 1144, whichmay determine whether and how to tune waveguide 1136 (e.g., to turn onor off an optical switch). Bonding pads 1148 may be connected to controllogic circuits 1144 through TSVs, and may also be connected to solderpads 1126 on PCB 620 through bonding wires 1142.

Utilizing a package as illustrated in FIG. 11 , some embodimentsimplement the clock signal generator in the PIC, whereas otherembodiments implement the clock signal generator utilizing elementspresent in both the PIC and the EIC. Thus, signal paths passing from thePIC to the EIC and from the EIC to the PIC can be utilized to provideboth electrical and optical or photonic functionality. Thus, FIG. 11illustrates an architecture that enables photodetector 670 to beintegrated with clock generator 660 in the PIC. This architecture alsoenables clock generator 660 to be implemented with some elements in theEIC as well as separate elements, for example, photodetector 670,implemented in the PIC. Thus, embodiments of the present inventionimplement the clock signal generator in a single semiconductor packagethat can be disposed in a cryostat for low temperature operation. One ofordinary skill in the art would recognize many variations,modifications, and alternatives.

Referring to FIG. 11 , in one embodiment, photodetector 1134 implementedin PIC die 1130 serves as photodetector 660 in FIG. 6 and the clocksignal generator (CSG) implemented in EIC die 1140 serves as clockgenerator 660. Thus, although FIG. 11 illustrates a number of componentsthat may not be utilized to implement elements of the clock generator,FIG. 11 illustrates an exemplary implementation. Additional descriptionrelated to integration of PIC dies and EIC dies in a single package isprovided in U.S. Provisional Patent Application No. 62/784,284, filed onDec. 21, 2018, the disclosure of which is hereby incorporated byreference in its entirety for all purposes.

It will be appreciated that the EIC and the PIC can be implemented on asingle substrate or different substrates as appropriate to theparticular application. Moreover, the EIC and PIC, if implemented ondifferent substrates, can be implemented in a single package. Thus,embodiments of the present invention utilize integration of elements,for example, onto the same substrate or the same package, that resultsin improvements and system performance not available using free-spacetechniques. One of ordinary skill in the art would recognize manyvariations, modifications, and alternatives.

The clock signals may be input to the multiplexer 650, as illustrated byclock signal 662, for controlling the operations of the multiplexer 650(e.g., controlling the timing of multiplexing). The clock signals mayalso be used, as illustrated by clock signal 664, to control theoperations of the other components of a photonic quantum computer, suchas the classical computer 140, the linear optical quantum circuit 120,and the reconfigurable single-photon measurement circuit 130 (asillustrated in FIG. 1A).

Because the clock signals are generated off of the excess pump photons,the clock signals may have the same repetition rate as that of the pumpphoton pulses (e.g., 10 GHz). As discussed above, the photon-pair source610 may generate photon pairs non-deterministically, and the probabilityof successfully generating a photon pair may be only 1-5% (e.g., onlyone photon pair is generated for every 20 pump photon pulses). Thus, ifthe clock signals are generated off the heralding signals generated bythe single photon detector 640, the clock signals would have been a lotslower. The method of generating clock signals as described above canprevent such a problem.

Referring to FIG. 6 , one photon-pair source 610 is utilized inconjunction with one clock generator 660, however, embodiments of thepresent invention are not limited to this particular implementation.

FIG. 13 is a simplified schematic diagram illustrating generation of aclock signal in conjunction with two or more photon-pair sources. In theexample shown in FIG. 13 , multiplexed sources are used but thesesources can be individual non-multiplexed non-deterministic sources orany combination of non-multiplexed and multiplexed sources. In thisexample, pump photon pulses (not shown) can be provided to any of themultiplexed sources, e.g., multiplexed sources 1303 a, . . . 1303 n, aportion of which are utilized to generate a corresponding clock signal1307 a, . . . , 1307 b, at each source, e.g., as described above inreference to FIGS. 6-9 . The clock signals are provided to a clockmediator 1305 which can generate a single master clock 1309 based on theindividual clock signals. There are many ways to generate such a masterclock. For example, the clock mediator can perform one or morediagnostic measurements on the individual clock signals and choose onebased on some criteria, such as Allan deviation, frequency jitter, phaserelative to photon generation time, and the like. In other embodiments,1305 can take the input clock signals and combine them via one or moremixers or other frequency reference generation circuits. In someembodiments the clock mediator 1305 itself can include one or morefrequency references that can be used for the generation of the masterclock.

FIG. 6 illustrates a single photon-pair source, however, it will beappreciated that systems can include multiple photon-pair sources. Thus,although FIG. 6 illustrates a clock signal for each photon-pair source,this is not required by the present invention and typically, one clocksignal will be generated in conjunction with multiple photon-pairsources. It should be noted that even if no photon-pair is produced byphoton-pair source 610, a clock signal can still be generated. Thus, aclock generator can be associated with every photon-pair source, withselection of clock signals performed, or only associated with one ofmany photon-pair sources.

According to some embodiments, the photon-pair source 610, the pumprejecter 620, the WDDM device 630, the single-photon detector 640, themultiplexer 650, the photodetector 670, and the clock generator 660 mayreside on a single chip that is placed inside a cryostat. Thephotodetector 670 may include a photodiode that is cryogenic-compatible(e.g., a Ge photodiode). Additional photon-pair sources (not shown inFIG. 6 ) may be multiplexed by the multiplexer 650 to form a pseudodeterministic single-photon source (e.g., as illustrated in FIG. 4 ).Because the clock signals are generated off of the excess pump photonsfrom the photon-pair source 610 that resides on the chip inside thecryostat, the clock signals may be in synch with the phases of thesingle photons generated by such a single-photon source.

In comparison, if the clock signals are generated directly from theelectrical signals that drive the pump photon source 602, which residesoutside the cryostat at room temperature, the clock signals may haverandom phase errors and drifts caused by the uncertain delays in theelectrical path due to the vast difference in temperatures. Such phaseerrors and drifts may render the clock signals unsuitable for the properoperation of the photonic quantum computer that has a tight timingtolerance. Thus, by generating the clock signals locally off of theexcess pump photons from the phone-pair source 610 that resides on thesame chip at the cryogenic temperature, as illustrated in FIG. 6 , theundesirable phase errors and drifts may be prevented or reduced.

FIG. 7 a schematic block diagram of a system for generating clocksignals for a photonic quantum computer according to some otherembodiments. Similar to the system illustrated in FIG. 6 , this systemmay include a pump photon source 702 that resides at room temperatureoutside a cryostat, and a photon-pair source 710 that resides inside thecryostat. The photon-pair source 710 is coupled to the pump photonsource 702 via a waveguide 704.

Similar to the photon-pair source 610, the photon-pair source 710 mayinclude a first waveguide 714, a resonator 712 optically coupled to thefirst waveguide 714, and a second waveguide 716 optically coupled to theresonator 712. A portion of the pump photons may be coupled from thefirst waveguide 714 into the resonator 712, while a remaining portion ofthe pump photons may exit the first waveguide 714 as non-coupled pumpphotons. The resonator 712 may convert some of the pump photons intopairs of signal photon and heralding photon. The converted photon pairs,as well as the excess pump photons that are not converted, may becoupled into the second waveguide 716 as output.

The output of the photon-pair source 710 may be coupled into a pumprejecter 720. The pump rejecter 720 separates the signal photon (S) andthe heralding photon (H) from the excess pump photons, for example viaspectral filtering. The excess pump photons may be absorbed by a beamdump (not shown). The signal photon and the heralding photon are in turnseparated by a wavelength division demultiplexing (WDDM) device 730. Theheralding photon may be detected by a single-photon detector 740, whichgenerates an electrical heralding signal. The heralding signal can beused by a multiplexer 750 for multiplexing signal photons generated by aplurality of photon-pair sources.

The system may further include a photodetector 770 coupled to a clockgenerator 760. Here, instead of taking the excess pump photons rejectedby the pump rejecter 720 as input, the photodetector 770 takes thenon-coupled pump photons from the first waveguide 714 of the photon-pairsource 710 as input, and generates electrical pulses to be input intothe clock generator 760. Because the photon-pair source 710 is placed onthe chip inside a cryostat, the clock signals generated in this way mayalso be in synch with the phases of the single photons generated by thesingle-photon source, and the undesirable phase errors and drifts may beprevented or reduced.

FIG. 8 a schematic block diagram of an alternative system for generatingclock signals for use by a single photon detector according to someembodiments. Similar to the system illustrated in FIG. 6 , this systemmay include a pump photon source 802 that resides at room temperatureoutside a cryostat, and a photon-pair source 810 that resides inside thecryostat. The photon-pair source 810 is coupled to the pump photonsource 802 via a waveguide 804.

Similar to the photon-pair source 610, the photon-pair source 810 mayinclude a first waveguide 814, a resonator 812 optically coupled to thefirst waveguide 814, and a second waveguide 816 optically coupled to theresonator 812. A portion of the pump photons may be coupled from thefirst waveguide 814 into the resonator 812, while a remaining portion ofthe pump photons may exit the first waveguide 814 as non-coupled pumpphotons. The resonator 812 may convert some of the pump photons intopairs of signal photon and heralding photon. The converted photon pairs,as well as the excess pump photons that are not converted, may becoupled into the second waveguide 816 as output.

The output of the photon-pair source 810 may be coupled into a pumprejecter 820. The pump rejecter 820 separates the signal photon (S) andthe heralding photon (H) from the excess pump photons, for example viaspectral filtering. The excess pump photons may be absorbed by a beamdump (not shown). The signal photon and the heralding photon are in turnseparated by a wavelength division demultiplexing (WDDM) device 830. Theheralding photon may be detected by a single-photon detector 840, whichgenerates an electrical heralding signal. The heralding signal can beused by a multiplexer 850 for multiplexing signal photons generated by aplurality of photon-pair sources.

The system may further include a photodetector 870 and a clock generator860. The photodetector 870 is optically coupled to the pump rejecter 820for receiving the excess pump photons rejected by the pump rejecter 820.The photodetector 870 may convert the excess pump photons intoelectrical pulses. The electrical pulses are in turn input into theclock generator 860, which generates clock signals from the electricalpulses. In some embodiments, the clock generator 860 may include anoptoelectronic amplifier that amplifies the electrical pulses generatedby the photodetector 870 to generate the clock signals.

The clock signals may be input to the multiplexer 850 for controllingthe operations of the multiplexer 850. For example, the clock signalsmay be used to control the timing of multiplexing. The clock signals mayalso be input to the single-photon detector 840 for controlling theoperation of the single-photon detector 840. For example, the clocksignals may be used to control when the single-photon detector 840should be turned on and off. The single-photon detector 840 may besusceptible to spurious noise in the environment. For example, asuperconducting nanowire single-photon detector is a very sensitivedevice and may generate dark counts in the absence of a detected photon.Thus, it may be helpful to turn on the single-photon detector 840 onlyat time intervals at which a photon may be expected.

FIG. 9 a schematic block diagram of an alternative system for generatingclock signals for use by a single photon detector according to someother embodiments. Similar to the system illustrated in FIG. 8 , thissystem may include a pump photon source 902 that resides at roomtemperature outside a cryostat, and a photon-pair source 910 thatresides inside the cryostat. The photon-pair source 910 is coupled tothe pump photon source 902 via a waveguide 904.

Similar to the photon-pair source 810, the photon-pair source 910 mayinclude a first waveguide 914, a resonator 912 optically coupled to thefirst waveguide 914, and a second waveguide 916 optically coupled to theresonator 912. A portion of the pump photons may be coupled from thefirst waveguide 914 into the resonator 912, while a remaining portion ofthe pump photons may exit the first waveguide 914 as non-coupled pumpphotons. The resonator 912 may convert some of the pump photons intopairs of signal photon and heralding photon. The converted photon pairs,as well as the excess pump photons that are not converted, may becoupled into the second waveguide 916 as output.

The output of the photon-pair source 910 may be coupled into a pumprejecter 920. The pump rejecter 920 separates the signal photon (S) andthe heralding photon (H) from the excess pump photons, for example viaspectral filtering. The excess pump photons may be absorbed by a beamdump (not shown). The signal photon and the heralding photon are in turnseparated by a wavelength division demultiplexing (WDDM) device 930. Theheralding photon may be detected by a single-photon detector 940, whichgenerates an electrical heralding signal. The heralding signal can beused by a multiplexer 950 for multiplexing signal photons generated by aplurality of photon-pair sources.

The system may further include a photodetector 970 and a clock generator960. Here, instead of taking the excess pump photons rejected by thepump rejecter 920 as input, the photodetector 970 takes the non-coupledpump photons from the first waveguide 914 of the photon-pair source 910as input, and generates electrical pulses to be input into the clockgenerator 960. Because the photon-pair source 910 is placed on the chipinside a cryostat, the clock signals generated in this way may also bein synch with the phases of the single photons generated by thesingle-photon source, and the undesirable phase errors and drifts may beprevented or reduced.

The clock signals may be input to the multiplexer 950 for controllingthe operations of the multiplexer 950. For example, the clock signalsmay be used to control the timing of multiplexing. The clock signals mayalso be input to the single-photon detector 940 for controlling theoperation of the single-photon detector 940. For example, the clocksignals may be used to control when the single-photon detector 940should be turned on and off.

FIG. 10 shows a simplified flowchart illustrating a method forgenerating clock signals for a photonic quantum computing systemaccording to some embodiments. As illustrated in FIG. 10 , the methodincludes generating, using a pump photon source disposed outside thecryostat, a plurality of pump photon pulses at a first repetition rate(1010) and converting, using a photon-pair source disposed inside thecryostat and optically coupled to the pump photon source via awaveguide, a first portion of each of a subset of the plurality of pumpphoton pulses into a photon pair (1012). The photon-pair source outputsa second portion of each pump photon pulse of the plurality of pumpphoton pulses. The photon pair can include a signal photon and aheralding photon, and one of the signal photon or the heralding photonis used by the quantum computing system as a qubit. The first portion ofeach of the subset of the plurality of pump photon pulses can beconverted into the photon pair non-deterministically.

The method also includes generating, using a photodetector disposedinside the cryostat, a plurality of electrical pulses by converting thesecond portion of each pump photon pulse of the plurality of pump photonpulses into a respective electrical pulse of the plurality of electricalpulses (1014) and generating, using a clock generator disposed insidethe cryostat and coupled to the photodetector, a plurality of clocksignals at the first repetition rate using the plurality of electricalpulses (1016).

In an embodiment, the photon-pair source, the photodetector, the clockgenerator, and the photonic quantum computing system are disposed on asingle chip placed inside the cryostat. The photon-pair source caninclude a first waveguide optically coupled to the pump photon sourcevia the waveguide for receiving the plurality of pump photon pulses, aresonator optically coupled to the first waveguide and comprising anonlinear optical material, and a second waveguide optically coupled tothe resonator. The method can further include coupling a portion of eachpump photon pulse of the plurality of pump photon pulses from the firstwaveguide into the resonator. The first portion of each of the subset ofthe plurality of pump photon pulses that is converted into the photonpair is among the portion and is converted by the nonlinear opticalmaterial of the resonator. The method can further include coupling thephoton pairs converted from the subset of the plurality of pump photonpulses by the resonator into the second waveguide. As an example, theresonator can include one or more ring resonators. In a particularembodiment, the second portion of each pump photon pulse of theplurality of pump photon pulses is among the portion and the methodfurther comprises coupling the second portion of each pump photon pulseof the plurality of pump photon pulses from the resonator into thesecond waveguide. In another particular embodiment, the method includesseparating, using a pump rejecter disposed inside the cryostat andoptically coupled to the second waveguide, the second portion of eachpump photon pulse of the plurality of pump photon pulses from the photonpairs and coupling the second portion of each pump photon pulse of theplurality of pump photon pulses into the photodetector to be convertedinto the plurality of electrical pulses. In one embodiment, the pumprejecter comprises a spectral filter.

The second portion of each pump photon pulse of the plurality of pumpphoton pulses can be among a remaining portion of each pump photon pulseof the plurality of pump photon pulses that is not coupled into theresonator. Accordingly, the method can include coupling the secondportion of each pump photon pulse of the plurality of pump photon pulsesfrom the first waveguide into the photodetector to be converted into theplurality of electrical pulses.

It should be appreciated that the specific steps illustrated in FIG. 10provide a particular method for generating clock signals for a photonicquantum computing system according to some embodiments. Other sequencesof steps may also be performed according to alternative embodiments. Forexample, alternative embodiments may perform the steps in a differentorder. Moreover, the individual steps may include multiple sub-stepsthat may be performed in various sequences as appropriate to theindividual step. Furthermore, additional steps may be added and somesteps may be removed depending on the particular applications. One ofordinary skill in the art would recognize many variations,modifications, and alternatives.

It will be apparent to those skilled in the art that substantialvariations may be made in accordance with specific implementations. Forexample, customized hardware might also be used, and/or particularelements might be implemented in hardware, software (including portablesoftware, such as applets, etc.), or both. Further, connection to othercomputing devices such as network input/output devices may be employed.

With reference to the appended figures, components that can includememory can include non-transitory machine-readable media. The terms“machine-readable medium” and “computer-readable medium” as used hereinrefer to any storage medium that participates in providing data thatcauses a machine to operate in a specific fashion. In embodimentsprovided hereinabove, various machine-readable media might be involvedin providing instructions/code to processors and/or other device(s) forexecution. Additionally or alternatively, the machine-readable mediamight be used to store and/or carry such instructions/code. In manyimplementations, a computer-readable medium is a physical and/ortangible storage medium. Such a medium may take many forms, including,but not limited to, non-volatile media, volatile media, and transmissionmedia. Common forms of computer-readable media include, for example,magnetic and/or optical media, punch cards, paper tape, any otherphysical medium with patterns of holes, a RAM, a programmable read-onlymemory (PROM), an erasable programmable read-only memory (EPROM), aFLASH-EPROM, any other memory chip or cartridge, a carrier wave asdescribed hereinafter, or any other medium from which a computer canread instructions and/or code.

The methods, systems, and devices discussed herein are examples. Variousembodiments may omit, substitute, or add various procedures orcomponents as appropriate. For instance, features described with respectto certain embodiments may be combined in various other embodiments.Different aspects and elements of the embodiments may be combined in asimilar manner. The various components of the figures provided hereincan be embodied in hardware and/or software. Also, technology evolvesand, thus, many of the elements are examples that do not limit the scopeof the disclosure to those specific examples.

It has proven convenient at times, principally for reasons of commonusage, to refer to such signals as bits, information, values, elements,symbols, characters, variables, terms, numbers, numerals, or the like.It should be understood, however, that all of these or similar terms areto be associated with appropriate physical quantities and are merelyconvenient labels. Unless specifically stated otherwise, as is apparentfrom the discussion above, it is appreciated that throughout thisspecification discussions utilizing terms such as “processing,”“computing,” “calculating,” “determining,” “ascertaining,”“identifying,” “associating,” “measuring,” “performing,” or the likerefer to actions or processes of a specific apparatus, such as a specialpurpose computer or a similar special purpose electronic computingdevice. In the context of this specification, therefore, a specialpurpose computer or a similar special purpose electronic computingdevice is capable of manipulating or transforming signals, typicallyrepresented as physical electronic, electrical, or magnetic quantitieswithin memories, registers, or other information storage devices,transmission devices, or display devices of the special purpose computeror similar special purpose electronic computing device.

Those of skill in the art will appreciate that information and signalsused to communicate the messages described herein may be representedusing any of a variety of different technologies and techniques. Forexample, data, instructions, commands, information, signals, bits,symbols, and chips that may be referenced throughout the abovedescription may be represented by voltages, currents, electromagneticwaves, magnetic fields or particles, optical fields or particles, or anycombination thereof.

Terms “and,” “or,” and “an/or,” as used herein, may include a variety ofmeanings that also is expected to depend at least in part upon thecontext in which such terms are used. Typically, “or” if used toassociate a list, such as A, B, or C, is intended to mean A, B, and C,here used in the inclusive sense, as well as A, B, or C, here used inthe exclusive sense. In addition, the term “one or more” as used hereinmay be used to describe any feature, structure, or characteristic in thesingular or may be used to describe some combination of features,structures, or characteristics. However, it should be noted that this ismerely an illustrative example and claimed subject matter is not limitedto this example. Furthermore, the term “at least one of” if used toassociate a list, such as A, B, or C, can be interpreted to mean anycombination of A, B, and/or C, such as A, B, C, AB, AC, BC, AA, AAB,ABC, AABBCCC, etc.

Reference throughout this specification to “one example,” “an example,”“certain examples,” or “exemplary implementation” means that aparticular feature, structure, or characteristic described in connectionwith the feature and/or example may be included in at least one featureand/or example of claimed subject matter. Thus, the appearances of thephrase “in one example,” “an example,” “in certain examples,” “incertain implementations,” or other like phrases in various placesthroughout this specification are not necessarily all referring to thesame feature, example, and/or limitation. Furthermore, the particularfeatures, structures, or characteristics may be combined in one or moreexamples and/or features.

In some implementations, operations or processing may involve physicalmanipulation of physical quantities. Typically, although notnecessarily, such quantities may take the form of electrical or magneticsignals capable of being stored, transferred, combined, compared, orotherwise manipulated. It has proven convenient at times, principallyfor reasons of common usage, to refer to such signals as bits, data,values, elements, symbols, characters, terms, numbers, numerals, or thelike. It should be understood, however, that all of these or similarterms are to be associated with appropriate physical quantities and aremerely convenient labels. Unless specifically stated otherwise, asapparent from the discussion herein, it is appreciated that throughoutthis specification discussions utilizing terms such as “processing,”“computing,” “calculating,” “determining,” or the like refer to actionsor processes of a specific apparatus, such as a special purposecomputer, special purpose computing apparatus or a similar specialpurpose electronic computing device. In the context of thisspecification, therefore, a special purpose computer or a similarspecial purpose electronic computing device is capable of manipulatingor transforming signals, typically represented as physical electronic ormagnetic quantities within memories, registers, or other informationstorage devices, transmission devices, or display devices of the specialpurpose computer or similar special purpose electronic computing device.

In the preceding detailed description, numerous specific details havebeen set forth to provide a thorough understanding of claimed subjectmatter. However, it will be understood by those skilled in the art thatclaimed subject matter may be practiced without these specific details.In other instances, methods and apparatuses that would be known by oneof ordinary skill have not been described in detail so as not to obscureclaimed subject matter. Therefore, it is intended that claimed subjectmatter not be limited to the particular examples disclosed, but thatsuch claimed subject matter may also include all aspects falling withinthe scope of appended claims, and equivalents thereof.

For an implementation involving firmware and/or software, themethodologies may be implemented with modules (e.g., procedures,functions, and so on) that perform the functions described herein. Anymachine-readable medium tangibly embodying instructions may be used inimplementing the methodologies described herein. For example, softwarecodes may be stored in a memory and executed by a processor unit. Memorymay be implemented within the processor unit or external to theprocessor unit. As used herein the term “memory” refers to any type oflong term, short term, volatile, nonvolatile, or other memory and is notto be limited to any particular type of memory or number of memories, ortype of media upon which memory is stored.

If implemented in firmware and/or software, the functions may be storedas one or more instructions or code on a computer-readable storagemedium. Examples include computer-readable media encoded with a datastructure and computer-readable media encoded with a computer program.Computer-readable media includes physical computer storage media. Astorage medium may be any available medium that can be accessed by acomputer. By way of example, and not limitation, such computer-readablemedia can comprise RAM, ROM, EEPROM, compact disc read-only memory(CD-ROM) or other optical disk storage, magnetic disk storage,semiconductor storage, or other storage devices, or any other mediumthat can be used to store desired program code in the form ofinstructions or data structures and that can be accessed by a computer;disk and disc, as used herein, includes compact disc (CD), laser disc,optical disc, digital versatile disc (DVD), floppy disk and blu-ray discwhere disks usually reproduce data magnetically, while discs reproducedata optically with lasers. Combinations of the above should also beincluded within the scope of computer-readable media.

In addition to storage on computer-readable storage medium, instructionsand/or data may be provided as signals on transmission media included ina communication apparatus. For example, a communication apparatus mayinclude a transceiver having signals indicative of instructions anddata. The instructions and data are configured to cause one or moreprocessors to implement the functions outlined in the claims. That is,the communication apparatus includes transmission media with signalsindicative of information to perform disclosed functions. At a firsttime, the transmission media included in the communication apparatus mayinclude a first portion of the information to perform the disclosedfunctions, while at a second time the transmission media included in thecommunication apparatus may include a second portion of the informationto perform the disclosed functions.

What is claimed is:
 1. A system for generating clock signals for aphotonic quantum computing system, the system comprising: a pump photonsource configured to generate a plurality of pump photon pulses at afirst repetition rate; a photon-pair source optically coupled to thepump photon source, the photon-pair source configured to: convert asubset of the plurality of pump photon pulses into photon pairs; outputthe photon pairs; and output a portion of each pump photon pulse of theplurality of pump photon pulses; a photodetector optically coupled tothe photon-pair source and configured to: receive the portion of eachpump photon pulse of the plurality of pump photon pulses; and convertingthe portion of each pump photon pulse of the plurality of pump photonpulses into a respective electrical pulse of a plurality of electricalpulses; and a clock generator electrically coupled to the photodetectorand configured to convert the plurality of electrical pulses into aplurality of clock signals at the first repetition rate.
 2. The systemof claim 1 wherein the photon-pair source, the photodetector, the clockgenerator, and the photonic quantum computing system are disposed insidea cryostat and the pump photon source is disposed outside the cryostat.3. The system of claim 1 wherein each of the photon pairs comprises asignal photon and a heralding photon, and one of the signal photon orthe heralding photon is used by the photonic quantum computing system asa qubit.
 4. The system of claim 1 further comprising a waveguideoptically coupled to the pump photon source and the photon-pair source.5. The system of claim 1 wherein each of the photon pairs comprises asignal photon and a heralding photon, and one of the signal photon orthe heralding photon is used by the photonic quantum computing system asa qubit.
 6. A system comprising: a pump photon source; a photon-pairsource optically coupled to the pump photon source, wherein thephoton-pair source is configured to: receive a plurality of pump photonpulses from the pump photon source; convert a first portion of theplurality of pump photon pulses into a photon pair; output the photonpair; and output a second portion of the plurality of pump photonpulses; and a photodetector optically coupled to the photon-pair sourceand configured to generate a plurality of electrical pulses in responseto detection of at least a portion of the plurality of pump photonpulses.
 7. The system of claim 6 further comprising a clock generatorcoupled to the photodetector, the clock generator configured to convertthe plurality of electrical pulses into a plurality of clock signals fora photonic quantum computing system.
 8. The system of claim 7 whereinthe photon-pair source and the photodetector are implemented in aphotonic integrated circuit (PIC) and the clock generator is implementedin an electronic integrated circuit (EIC).
 9. The system of claim 8wherein the PIC and EIC are fusion bonded.
 10. The system of claim 7wherein the photon-pair source, the photodetector, and the clockgenerator are implemented on a same substrate structure.
 11. The systemof claim 10 wherein the same substrate structure comprises a fused PICand EIC.
 12. The system of claim 7 wherein the photon-pair source, thephotodetector, the clock generator, and the photonic quantum computingsystem are disposed on a single chip disposed inside a cryostat.
 13. Thesystem of claim 12 wherein the pump photon source is disposed outsidethe cryostat.
 14. The system of claim 6 wherein the photon paircomprises a signal photon and a heralding photon, and one of the signalphoton or the heralding photon is used by a quantum computing system asa qubit.
 15. The system of claim 6 wherein the photon-pair sourceconverts the first portion of the plurality of pump photon pulses intothe photon pair non-deterministically.
 16. The system of claim 6 whereinthe photon-pair source comprises: a first waveguide for receiving theplurality of pump photon pulses generated by the pump photon source; aresonator optically coupled to the first waveguide so that a portion ofeach pump photon pulse of the plurality of pump photon pulses is coupledinto the resonator, the resonator comprising a nonlinear opticalmaterial for converting the first portion of the plurality of pumpphoton pulses into the photon pair; and a second waveguide opticallycoupled to the resonator so that the photon pair converted from theplurality of pump photon pulses are coupled thereto.
 17. The system ofclaim 16 wherein the resonator comprises one or more ring resonators.18. The system of claim 16 wherein the second portion of the pluralityof pump photon pulses is coupled into the second waveguide and output bythe second waveguide.
 19. The system of claim 18 further comprising apump rejecter optically coupled to the second waveguide of thephoton-pair source, the pump rejecter configured to: receive the photonpair and the second portion of the plurality of pump photon pulses;output the photon pair through a first output port; and output thesecond portion of the plurality of pump photon pulses through a secondoutput port optically coupled to the photodetector.
 20. The system ofclaim 19 wherein the pump rejecter comprises a spectral filter.